Table 2
Outflow energetics for the two CO transitions.
| CO J = 3–2 | CO J = 2–1 | CO J = 2–1 | ||
| Integrated | Filtered | |||
|
|
||||
| M (10-6 M⊙) | 5.7 ± 0.06 | 73.1 ± 0.8 | 24.6 ± 0.3 | |
| V (km s-1) | −18.6 ± 0.1 | −18.6 ± 0.3 | −18.9 ± 0.5 | |
| P(10-5 M⊙ km s-1) | 10.7 ± 0.1 | 136.0 ± 3.5 | 46.4 ± 4.6 | |
| E (1040 erg) | 1.98 ± 0.04 | 25.1 ± 1.0 | 8.7 ± 0.5 | |
|
|
||||
| Wind kinematic age = 400 yr | ||||
|
|
||||
| F a | 2.7 ± 0.3 | 34.0 ± 4 | 11.5 ± 2 | |
| L (10-3 L⊙) | 0.41 ± 0.05 | 5.2 ± 0.7 | 1.8 ± 0.3 | |
| Ṁout (10-8 M⊙ yr-1) | 1.4 ± 0.2 | 18.3 ± 2 | 6.2 ± 0.7 | |
Notes. The first CO J = 2–1 column is derived from integrating over all of the CO J = 2–1 emission, while the second is derived from the data that was filtered to sample the same spatial scales as the Band 7 data. This “Filtered” column is more directly comparable to the J = 3–2 data. The quoted uncertainties come from the uncertainties in the fluxes, propagated through the equations in quadrature. Note that the quoted velocity is blue shifted with respect to the source velocity of 5.8 km s-1.
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